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A wire of length 1 m and radius 10^-3m i...

A wire of length 1 m and radius `10^-3`m is carrying a heavy current and is assumed to radiate as a black body. At equilibrium, its temperature is 900 K while that of surrounding is 300 K. The resistivity of the material of the wire at 300 K is `pi^@xx10^-8` ohm m and its temperature coefficient of resistance is `7.8xx10^(-3)//C` (stefan's constant`sigma=5.68xx10^-8W//m^(2) K^(2)`.
Heat radiated per second by the wire is nearly

A

23 W

B

230 W

C

2300 W

D

23000 W

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The correct Answer is:
To solve the problem of finding the heat radiated per second by the wire, we will use the Stefan-Boltzmann law, which states that the power radiated by a black body per unit area is proportional to the fourth power of its temperature. The formula for the power radiated by a black body is given by: \[ P = \sigma A (T^4 - T_{surrounding}^4) \] Where: - \( P \) is the power radiated (in watts), - \( \sigma \) is the Stefan-Boltzmann constant (\( 5.68 \times 10^{-8} \, \text{W/m}^2 \, \text{K}^4 \)), - \( A \) is the surface area of the wire (in m²), - \( T \) is the temperature of the wire (in K), - \( T_{surrounding} \) is the temperature of the surroundings (in K). ### Step-by-Step Solution: 1. **Identify the given values:** - Length of the wire, \( L = 1 \, \text{m} \) - Radius of the wire, \( r = 10^{-3} \, \text{m} \) - Temperature of the wire, \( T = 900 \, \text{K} \) - Temperature of the surroundings, \( T_{surrounding} = 300 \, \text{K} \) - Stefan-Boltzmann constant, \( \sigma = 5.68 \times 10^{-8} \, \text{W/m}^2 \, \text{K}^4 \) 2. **Calculate the surface area of the wire:** The surface area \( A \) of a cylindrical wire can be calculated using the formula: \[ A = 2 \pi r L \] Substituting the values: \[ A = 2 \pi (10^{-3}) (1) = 2 \pi \times 10^{-3} \, \text{m}^2 \] 3. **Calculate \( T^4 \) and \( T_{surrounding}^4 \):** - Calculate \( T^4 \): \[ T^4 = (900)^4 = 6.561 \times 10^{8} \, \text{K}^4 \] - Calculate \( T_{surrounding}^4 \): \[ T_{surrounding}^4 = (300)^4 = 8.1 \times 10^{6} \, \text{K}^4 \] 4. **Substitute values into the power formula:** Now we can substitute \( A \), \( T^4 \), and \( T_{surrounding}^4 \) into the power formula: \[ P = \sigma A (T^4 - T_{surrounding}^4) \] \[ P = 5.68 \times 10^{-8} \times (2 \pi \times 10^{-3}) \times (6.561 \times 10^{8} - 8.1 \times 10^{6}) \] 5. **Calculate the difference \( T^4 - T_{surrounding}^4 \):** \[ T^4 - T_{surrounding}^4 = 6.561 \times 10^{8} - 8.1 \times 10^{6} \approx 6.4809 \times 10^{8} \] 6. **Calculate the power \( P \):** \[ P = 5.68 \times 10^{-8} \times (2 \pi \times 10^{-3}) \times (6.4809 \times 10^{8}) \] \[ P \approx 5.68 \times 10^{-8} \times 6.2832 \times 10^{-3} \times 6.4809 \times 10^{8} \] \[ P \approx 230 \, \text{W} \] ### Final Answer: The heat radiated per second by the wire is approximately **230 watts**.

To solve the problem of finding the heat radiated per second by the wire, we will use the Stefan-Boltzmann law, which states that the power radiated by a black body per unit area is proportional to the fourth power of its temperature. The formula for the power radiated by a black body is given by: \[ P = \sigma A (T^4 - T_{surrounding}^4) \] Where: - \( P \) is the power radiated (in watts), - \( \sigma \) is the Stefan-Boltzmann constant (\( 5.68 \times 10^{-8} \, \text{W/m}^2 \, \text{K}^4 \)), - \( A \) is the surface area of the wire (in m²), ...
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